/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 73 A \(12.6-\mathrm{V}\) car batter... [FREE SOLUTION] | 91Ó°ÊÓ

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A \(12.6-\mathrm{V}\) car battery with negligible internal resistance is connected to a series combination of a \(3.2-\Omega\) resistor that obeys Ohm's law and a thermistor that does not obey Ohm's law but instead has a current- voltage relationship \(V=\alpha I+\beta I^{2},\) with \(\alpha=3.8 \Omega\) and \(\beta=1.3 \Omega / \mathrm{A}\) . What is the current through the \(3.2-\Omega\) resistor?

Short Answer

Expert verified
The current through the 3.2-ohm resistor is approximately 1.2 A.

Step by step solution

01

Understanding the Circuit Arrangement

The circuit includes a 12.6-V battery connected in series with a 3.2-ohm resistor and a thermistor. The key here is that the same current flows through both the resistor and the thermistor since they are in series.
02

Apply Ohm's Law to the Resistor

For the 3.2-ohm resistor, we use Ohm's Law, which is \( V = IR \). Here, \( I \) is the current we're trying to find, and \( V \) is the voltage drop across the resistor, which is equal to \( 3.2I \) as per Ohm's Law.
03

Establish the Voltage-Current Relationship for the Thermistor

The thermistor has a voltage-current relationship given by \( V = \alpha I + \beta I^{2} \). Substituting \( \alpha = 3.8 \Omega \) and \( \beta = 1.3 \Omega/\mathrm{A} \), the equation becomes \( V_t = 3.8I + 1.3I^{2} \).
04

Formulate the Total Voltage Equation

As the battery provides a total voltage of 12.6 V, the sum of the voltage drops across the resistor and the thermistor equals this total voltage: \( 3.2I + (3.8I + 1.3I^{2}) = 12.6 \). Simplifying gives us the equation: \( 7.0I + 1.3I^2 = 12.6 \).
05

Solve the Quadratic Equation for Current

Rearrange the equation to standard quadratic form: \( 1.3I^2 + 7.0I - 12.6 = 0 \). Using the quadratic formula \( I = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \), where \( a = 1.3 \), \( b = 7.0 \), and \( c = -12.6 \), calculate to find \( I \).
06

Calculate and Simplify

Calculate the discriminant \( b^2 - 4ac = 7^2 - 4 \times 1.3 \times (-12.6) \). Compute the value using the quadratic formula: \( I = \frac{-7 \pm \sqrt{49 + 65.52}}{2 \times 1.3} \). Simplify to find \( I \approx 1.2 \mathrm{A} \) - only the positive value is physically meaningful.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Understanding Series Circuits
In a series circuit, components are connected end-to-end so that the current flows through each component without branching off. This arrangement ensures that the current is the same at all points in the circuit. In the provided exercise, the circuit consists of a 12.6-V battery connected in series with a 3.2-ohm resistor and a thermistor. The key characteristic of a series circuit is that the total voltage supplied by the battery is equal to the sum of the voltage drops across each component in the circuit.

This means:
  • The current across each component is identical, so calculating the current once will give us its value everywhere in the circuit.
  • The voltage drop across each component adds up to the total battery voltage.
  • Therefore, Ohm's Law can be applied to each component individually and then summed to establish equations that reflect the entire circuit.
Understanding this concept is crucial because it allows for predicting how changes in one component affect the entire circuit's behavior.
Using Quadratic Equations for Circuit Analysis
Quadratic equations commonly appear in physics and engineering problems, especially when dealing with non-linear components like the thermistor in our example. Here, the challenge of calculating the total voltage in a series circuit involving a non-linear device leads to a quadratic equation. We derive this from the relationship:
  • Resistor voltage: \( V = IR \)
  • Thermistor voltage: \( V = \alpha I + \beta I^2 \)
  • Total voltage from the battery: 12.6 V
The voltage drops add up to the total battery voltage, leading us to the quadratic equation \( 1.3I^2 + 7.0I - 12.6 = 0 \). Solving this equation requires finding the roots using the quadratic formula:\[I = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}\]In our exercise, solving this equation gives us the current value flowing through the series circuit, emphasizing the importance of quadratic equations in solving non-linear system relationships.
Calculating Current in Complex Circuits
Current calculation is a fundamental task in electrical studies, especially with components like resistors and thermistors. Ohm's Law, \( V = IR \), governs the relationship for linear resistors. However, the thermistor's current-voltage relationship introduces complexity with terms \( \alpha I + \beta I^2 \).

In this exercise:
  • We recognize that current, \( I \), is consistent across the series circuit.
  • The voltage equation combines terms from both resistor and thermistor: \( 3.2I + (3.8I + 1.3I^{2}) = 12.6 \).
  • Solving involves algebraic manipulation and applying the quadratic formula where precise current values are found, showcased by solving \( 1.3I^2 + 7I - 12.6 = 0 \).
By calculating the roots of this equation, we find the valid physical current approximately as 1.2 A. This calculation is critical in understanding how current behaves in circuits with mixed linear and non-linear characteristics.

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Most popular questions from this chapter

A lightning bolt strikes one end of a steel lightning rod, producing a \(15,000-\mathrm{A}\) current burst that lasts for 65\(\mu\) s. The rod is 20 \(\mathrm{m}\) long and 1.8 \(\mathrm{cm}\) in diameter, and its other end is connected to the ground by 35 \(\mathrm{m}\) of \(8.0-\mathrm{mm}\) -diameter copper wire (a) Find the potential difference between the top of the steel rod and the lower end of the copper wire during the current burst. (b) Find the total energy deposited in the rod and wire by the current burst.

You apply a potential difference of 4.50 \(\mathrm{V}\) between the ends of a wire that is 2.50 \(\mathrm{m}\) in length and 0.654 \(\mathrm{mm}\) in radius. The resulting current through the wire is 17.6 \(\mathrm{A}\) . What is the resistivity of the wire?

A Nonideal Ammeter. Unlike the idealized ammeter described in Section 25.4, any real ammeter has a nonzero resistance. (a) An ammeter with resistance \(R_{A}\) is connected in series with a resistor \(R\) and a battery of emf \(\mathcal{E}\) and internal resistance \(r .\) The current measured by the ammeter is \(I_{A}\) . Find the current through the circuit if the ammeter is removed so that the battery and the resistor form a complete circuit. Express your answer in terms of \(I_{A}, r, R_{A},\) and \(R\) . The more "ideal" the ammeter, the smaller the difference between this current and the current \(I_{A}\) . (b) If \(R=3.80 \Omega\) , \(\mathcal{E}=7.50 \mathrm{V},\) and \(r=0.45 \Omega,\) find the maximum value of the ammeter resistance \(R_{A}\) so that \(I_{A}\) is within 1.0\(\%\) of the current in the circuit when the ammeter is absent. (c) Explain why your answer in part (b) represents a maximum value.

A \(25.0-\Omega\) bulb is connected across the terminals of a \(12.0-\mathrm{V}\) battery having 3.50\(\Omega\) of internal resistance. What percentage of the power of the battery is dissipated across the internal resistance and hence is not available to the bulb?

The potential difference across the terminals of a battery is 8.4 \(\mathrm{V}\) when there is a current of 1.50 \(\mathrm{A}\) in the battery from the negative to the positive terminal. When the current is 3.50 \(\mathrm{A}\) in the reverse direction, the potential difference becomes 9.4 \(\mathrm{V}\) . (a) What is the internal resistance of the battery? (b) What is the emf of the battery?

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